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Transcript
Real Analog - Circuits 1
Chapter 4: Lab Projects
4.6.1: Maximum Power Transfer
Overview:
This assignment involves the maximum power transfer theorem. We will inappropriately attempt to maximize
the power delivered to a load resistor by, in some sense, re-defining the source circuit.
Before beginning this lab, you should be able to:


Create a Thevenin equivalent of an arbitrary
linear circuit
Determine the load resistance necessary to
draw the maximum power from a circuit
After completing this lab, you should be able to:

Compare measured voltages and currents in an
electrical circuit with predictions based on
superposition techniques
This lab exercise requires:



Analog Discovery module
Digilent Analog Parts Kit
Digital multimeter
Symbol Key:
Demonstrate circuit operation to teaching assistant; teaching assistant should initial lab notebook and
grade sheet, indicating that circuit operation is acceptable.
Analysis; include principle results of analysis in laboratory report.
Numerical simulation (using PSPICE or MATLAB as indicated); include results of MATLAB
numerical analysis and/or simulation in laboratory report.
Record data in your lab notebook.
© 2012 Digilent, Inc.
1
Real Analog – Circuits 1
Lab Project 4.6.1: Maximum Power Transfer
General Discussion:
Thévenin’s theorem tells us that the power delivered to a load is maximized if the load resistance is equal to the
Thevenin resistance of the circuit supplying the power. It is often desirable to design our load resistance to draw
the maximum power from a source circuit – this results in the minimum power being lost as heat dissipated
within the source circuit. In this case, the load is said to be matched to the source.
In this lab exercise, we will attempt to maximize power transfer to a load by modifying the source circuit. (We
will, in essence, attempt to match the source to the load rather than the other way around.) We will see that this
approach is inappropriate; the maximum power transfer theorem does not apply in “reverse”.
Pre-lab:
Our goal is to transfer the maximum amount of power to a 2.2k load resistor. The circuit schematic
shown in Figure 1 illustrates connection of the load resistor directly to a non-ideal source. Assuming
that the source resistance RS is much less than the load resistance RL (e.g. RS << RL), calculate the
power delivered to the load resistor.
RS
+
VS
+
-
RL
Vout
-
Source
Figure 1. “Loaded” non-ideal source.
We know that the maximum power will be delivered to the load resistor of Figure 1 if RL = RS. In this lab
assignment, we do not have the luxury of changing our load, but we can re-define our “source”. Add a resistance
to the “source” as shown in Figure 2; note that the “source” resistance and the load resistance are now the same.
Calculate the power delivered to the load resistor for this case and compare this power delivery to that of Figure 1.
RS
RL-RS
+
VS
+
-
RL
Vout
-
Modified “source”
Figure 2. “Loaded” source with modified source resistance.
© 2012 Digilent, Inc.
2
Real Analog – Circuits 1
Lab Project 4.6.1: Maximum Power Transfer
Lab Procedures:
1. Implement the circuit of Figure 1 with RL = 2.2k and VS = 5V. Use a 5k potentiometer to
implement RL; we will vary the load resistance in step 3 below. Measure VOUT and calculate the
power delivered to the load. Compare this power delivery with the power delivered to the 25
resistor in lab assignment 2.4. Are the relative powers delivered consistent with your estimate of
the source resistance determined in lab assignment 2.4 and the maximum power theorem?
2. Modify the “source” according to Figure 2, with RL = 2.2k and VS = 5V. You may assume that
RS << RL, so that RL – RS  RL = 2.2k. You may use a fixed 2.2k resistor to implement the
added source resistance RL – RS. Measure VOUT and calculate the power delivered to the load. Is
this power consistent with your previous results and the maximum power theorem?
3. In step 1 above, we (hopefully) realized that attempting to modify the source resistance does not
result in the maximum overall power transfer to the load. In this step, we will see that the
modified circuit of step 2 does provide the maximum power transfer for that value of source
resistance. (That maximum power is just less than the maximum possible power transfer if we
vary the source resistance.)
In order to do this, measure VOUT and calculate the power delivered to the load for at least five
values of load resistance over a range of (approximately) 1k < RL < 4k. Use VS = 5V, as in
steps 1 and 2. (This is easy if the load resistance is implemented with a potentiometer, as
recommended in step 1 above.) Plot the power delivered to the load vs. the load resistance. Are
your results consistent with the maximum power theorem?
4. Demonstrate operation of your circuit to the Teaching Assistant. Have the TA initial the
appropriate page(s) of your lab notebook and the lab checklist.
© 2012 Digilent, Inc.
3